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1  prolyl peptide bonds, and that unfolding is multiexponential.
2    In all mutants, fluorescence kinetics are multiexponential.
3 nated, as the luminescence decays were still multiexponentials.
4 been hampered by the heterogeneous nature of multiexponential 2AP intensity decays observed across po
5 e membrane association kinetics of pHLIP are multiexponential and are consistent with a parallel memb
6 than protein folding, the kinetics are often multiexponential, and the observed relaxation times are
7 ity of states measurements indicate that the multiexponential behavior that is often observed in inte
8 In monellin, the fluorescence decay displays multiexponential character with decay times of 1.2 and 1
9 PR frequencies requires a consideration of a multiexponential correlation function.
10                      However, TRFS relies on multiexponential data fitting to derive fluorescence lif
11 ted the Iterative Thresholding Algorithm for Multiexponential Decay (ITAMeD), which employs the l(1)-
12                                  Analysis of multiexponential decay has remained a topic of active re
13      To experimentally simulate fluorescence multiexponential decay kinetics, we varied the concentra
14 in chemical reactions and species displaying multiexponential decay kinetics.
15 tically dense samples that exhibit single or multiexponential decay kinetics.
16 of 2A(g)(-) symmetry in 39 fs, followed by a multiexponential decay to the ground state on the 1-100
17 th the excited-state relaxation exhibiting a multiexponential decay with well-defined rate constants.
18  formation, has a rapid risetime and complex multiexponential decay.
19 sed with potency, and slow components in the multiexponential decays became more prominent.
20 his method can be used to resolve single and multiexponential decays in the presence of short lifetim
21 e luminescence decay kinetics transform from multiexponential decays typical of nanocrystalline semic
22 phase with tau = 10 msec, followed by a slow multiexponential decline.
23 gand competition at high concentrations, and multiexponential dissociation arising from differential
24                                              Multiexponential dynamics were observed in previous ultr
25 pproximately L(2.17+/-0.17) when analyzed by multiexponential fit.
26 of the components due to inherently instable multiexponential fits or data inversion procedures.
27                                              Multiexponential fitting gave the following apparent lif
28                                        Using multiexponential fitting of fluorescence recovery curves
29 e the decays of coincident spectral peaks by multiexponential fitting, but the well-known fundamental
30 is of singular value decomposition (SVD) and multiexponential fitting, three apparent lifetimes were
31 alysis, an alternate approach to traditional multiexponential fitting, to evaluate photoreceptor two-
32 ed singular value decomposition analysis and multiexponential fitting.
33 analyzed by singular-value decomposition and multiexponential fitting.
34 lyzed using singular value decomposition and multiexponential fitting.
35 to perform tailored and fit-free analysis of multiexponential fluorescence decay curves.
36 sis, photosystem II (PSII), exhibits complex multiexponential fluorescence decay kinetics that for de
37 th a single tryptophan residue that exhibits multiexponential fluorescence decay kinetics, was also e
38             In vesicle containing solutions, multiexponential fluorescence decays imply separate solu
39 fibers were formed under conditions in which multiexponential folding kinetics is observed in other s
40 a fluorescent ATP analogue is fitted using a multiexponential function.
41                                              Multiexponential functions were fit iteratively to the t
42                                              Multiexponential functions were iteratively fit to each
43                                              Multiexponential functions were iteratively fit to each
44 ear least squares fits of the tissue data to multiexponential functions.
45 simulations of RyR clusters that utilize the multiexponential gating model produce infrequent Ca(2+)
46  for many common distributions (exponential, multiexponential, Gaussian, etc.), as well as user-speci
47    Both reactions can be described by either multiexponential kinetics, which would lead to apparent
48                                     Use of a multiexponential model enabled us to reduce the gap betw
49 (CT) distributions, and an extension of this multiexponential model that also includes experimentally
50                                 We show that multiexponential models provide the necessary tool to ob
51          The physical nature of the observed multiexponential or stretched-exponential ET dynamics in
52 eans of circumventing conventional limits on multiexponential parameter estimation.
53                                    We find a multiexponential process with approximately two-thirds o
54              Kv4.3 inactivation is a complex multiexponential process, which can occur from both clos
55 pment that can be empirically described with multiexponential regression models, which suggests that
56     The residence times were determined from multiexponential regression of organ region-of-interest
57 d activity coefficients were determined from multiexponential regression of organ region-of-interest
58         Residence times were determined from multiexponential regression of organ region-of-interest
59 sociated motor proteins, and lead to complex multiexponential relaxations that occur over a wide rang
60                             The kinetics was multiexponential, showing that the conformational ensemb
61                 For TRFS data, not only pure multiexponential tail information but also shorter time
62 duction in the LSS response, and exhibited a multiexponential time course of activation.
63 ealed synaptic currents that decayed along a multiexponential time course, reflecting receptors conta
64 solve this problem, we tested the utility of multiexponential versus continuous Lorentzian lifetime d
65  is especially challenging when the decay is multiexponential with an unknown number of components.